Wireless traction battery force sensor
US-2017331160-A1 · Nov 16, 2017 · US
US9528896B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9528896-B2 |
| Application number | US-201313839238-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 15, 2013 |
| Priority date | Mar 15, 2013 |
| Publication date | Dec 27, 2016 |
| Grant date | Dec 27, 2016 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A cylindrical quartz crystal transducer that exhibits a low probability of twinning, and uses a combination of resonator signal inputs at the B-mode and C-mode frequencies to calculate resonator temperature. Crystallographic orientations are disclosed where combinations of B-mode and C-mode resonant frequencies exist that are sufficiently independent of pressure to enable accurate calculation of temperature under transient conditions. Such a transducer is usable at higher pressures and temperatures than conventional quartz pressure transducers. Furthermore, because the structure allows a choice of crystallographic orientation, other characteristics of the transducer, such as increased pressure sensitivity and activity dip-free operation, may be optimized by varying crystallographic orientation.
Opening claim text (preview).
What is claimed is: 1. A dual-mode pressure transducer, comprising: a quartz crystal structure having a crystallographic orientation, wherein the quartz crystal structure comprises: a double cut comprising: a first cut having a first angular displacement (phi) about the X-axis of 26°; and a second cut having a second angular displacement (theta) about the Z-axis between 33° and 34°; a substantially cylindrical body having a longitudinal bore; and a disc-shaped resonator carried by the body and extending transversely across the longitudinal bore; and an electronics assembly in communication with the quartz crystal structure, the electronics assembly configured to: drive the resonator; receive signal inputs from the resonator from a non-fundamental B-mode resonant frequency primarily dependent on temperature; receive other signal inputs from the resonator from a non-fundamental C-mode resonant frequency primarily dependent on pressure; and calculate pressure-independent temperature under transient conditions using a combination of the signal inputs and the other signal inputs to compensate for the pressure determined from the non-fundamental C-mode resonant frequency. 2. The pressure transducer of claim 1 , wherein the disc-shaped resonator is integral with the body, and further including end caps secured to the body across opposing ends of the longitudinal bore. 3. The pressure transducer of claim 1 , wherein the body comprises first and second end caps, each end cap defining a portion of the longitudinal bore on opposing sides of the disc-shaped resonator and having the disc-shaped resonator secured therebetween. 4. The pressure transducer of claim 1 , wherein the resonator is a 3 rd overtone blank with a contour of 2.5 diopters on both sides. 5. A method of measuring a temperature-compensated pressure using a quartz crystal structure, the method comprising: stimulating, under transient temperature conditions, the disc-shaped resonator of the quartz crystal structure of the dual-mode pressure transducer of claim 1 under external pressure applied to the quartz crystal structure to provide signal inputs from a non-fundamental B-mode resonant frequency and a non-fundamental C-mode resonant frequency; and using a combination of the signal inputs to compensate a pressure determined from the non-fundamental C-mode resonant frequency signal input. 6. The method of claim 5 , wherein using a combination of the signal inputs comprises using a sum of the signal inputs. 7. The method of claim 5 , wherein the non-fundamental B-mode resonant frequency and the non-fundamental C-mode resonant frequency is the 3 rd harmonic of each mode. 8. The method of claim 5 , further comprising determining a change in temperature with the following equation: Δ T = ( f C + Kf B - f C 1 - Kf B 1 ) ( f C 1 C T + Kf B 1 B T ) . 9. The method of claim 5 , further comprising determining a change in pressure with the following equation: Δ P = C T C P ( f C 1 C P + Kf B 1 B P ) (
Related publications grouped by family.
Answers are generated from the same data shown on this page.